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NEW_Accomplishments.indd - IRIS

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2006 <strong>IRIS</strong> 5-YEAR PROPOSAL UPWELLING AND DOWNWELLING<br />

Seismic Evidence for Hotspot-Induced Buoyant Flow Beneath the<br />

Reykjanes Ridge<br />

James B. Gaherty • Lamont-Doherty Earth Observatory of Columbia University<br />

Volcanic hotspots and mid-ocean ridge spreading centers are the surface expressions of upwelling in Earthʼs mantle convection<br />

system, and their interaction provides unique information on upwelling dynamics. I investigated the influence of the<br />

Iceland hotspot on the adjacent mid-Atlantic spreading center (the Reykjanes Ridge, RR) using seismic surface waves from<br />

mid-Atlantic ridge earthquakes recorded at the Global Seismic Network station BORG and stations of the ICEMELT and<br />

HOTSPOT PASSCAL deployments (left). The surface waves from these events travel along and adjacent to the RR, and the<br />

travel times of these waves are sensitive to the average crust and upper-mantle velocity along each path. These delay times<br />

were inverted for age-dependent models of radial anisotropy (right). The models show a distinct pattern of shear anisotropy<br />

(∆V S ), with negative values (V SV > V SH ) above about 100 km depth, and positive values between about 100-200 km depth.<br />

This pattern of anisotropy is unlike that in comparable oceanic models, which display ∆V S > 0 throughout the upper 200 km<br />

of the mantle. This anisotropy suggests that the hotspot induces buoyancy-driven upwelling in the mantle beneath the ridge.<br />

In this model, the melt-zone upwelling is driven by buoyancy associated with retained melt, melt residuum, and/or locally hot<br />

(left) Bathymetric map of the North Atlantic study region. Surface waves of earthquakes (open circles) from the Reykjanes<br />

Ridge (RR) and the Gibbs Fracture Zone (GFZ) were recorded on Iceland at BORG and the ICEMELT and HOT-<br />

SPOT stations (inverted and upright triangles, respectively). Seafloor age is contoured at 20 Ma intervals. (right) Upper-mantle<br />

shear-velocity models of the Reykjanes region. Left panel displays mean shear speed (vS = (vSH+vSV)/2),<br />

while right panel displays shear anisotropy (vS = (vSH-vSV)/vS) in percent). Three age regions are shown: 0-5 Ma<br />

(short dash), 10-15 Ma (long dash), and 25-40 Ma (solid). Also shown (dash-dot lines) are shear-velocity models for<br />

Pacific upper-mantle (Nishimura and Forsyth, 1989).<br />

mantle. Such models produce a tight circulation within the melting zone, and as the mantle material moves out of the spreading<br />

center, a near-vertical fabric associated with the downgoing limb of the circulation is retained in the off-axis lithosphere<br />

to a depth of ~60-100 km. This result suggests that buoyancy-driven upwelling is an important component of ridge dynamics,<br />

especially in environments where passive sea-floor spreading is too slow to accommodate melt production. It also implies<br />

that the anisotropic structure of oceanic lithosphere may not be as simple as inferred through studies from the fast-spreading<br />

Pacific ridges, and that this structure holds important clues to ridge and plume dynamics.<br />

Gaherty, J.B., Seismic evidence for hotspot-induced buoyant flow beneath the Reykjanes Ridge, Science, 293, 1645-1647, 2001.<br />

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